Stories of the Stars: Canus Major. Artwork by Frank Paul
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Starmaps seem so crystal pure and elegant. But reality is far more
messy. The night sky seem to be decorated with static stars firmly nailed
to the firmament, but reality is closer to an explosion in a glitter factory.
The only reason they seem to be stationary is because (1) space is so freaking huge, (2) stars move (relatively) slowly, and (3) human beings think that ten thousand years is a little to long to sit and watch the action. Some planetarium computer programs have an option to show how distorted the constellations appear millions of years in the past ( as seen by the dinosaurs ) or millions of years in the future ( as seen by all the mutant rats and cockroaches ). |
And in times gone by, a star that was quite close to another could now be quite remote. This can have implications for young upstart interstellar explorers who want to loot ancient high-tech goodies in the ruins of long gone empires. What used to be a nice compact empire half a million years ago is now spread out over a large section of the spiral arm.
But again I warn you, the math is not going to be easy.
( Thanks to Thomas York for the first half of these equations, visit his web site. And double thanks to Richard Powell for the other half, do check out his Atlas of the Universe )
And if you want more terse but lucid instructions, go to Armchair Astrometrist.
Information about the motion of a star is generally given in terms of Radial Velocity and Proper Motion. Why? Because they are the easiest things for an astronomer to measure, that's why.
Any star's motion ( or vector ) is a complicated thing, but any vector can be split into two vectors, much in the same way that any line can be drawn using the two controls of an Etch-a-Sketch. So one knob will be the Radial Velocity knob, and the other the Proper Motion knob. The vector is called the Space Velocity.
Radial velocity is simply how fast the star is approaching or running away from the Sun ( the rate the RV knob is being turned ). It is easy to measure this with a spectroscope, as the star's spectrum is under the influence of the dreaded Doppler Effect. ( I'm not going to attempt to explain this here, but five minutes with a web searcher should turn up a few tutorials ). Most star's RV's are less than 100 kilometers per second, they are typically from 10 to 40 km/s. Positive values mean the star is receeding from the Sun, negative values are approaching.
Proper motion is how fast the star seems to move left or right in the sky, as viewed from the Sun ( the rate of the PM knob is being turned ). It is measured by taking photographs of stars from year to year and painstakingly measuring how much the image moves. The poor astronomer's task is complicated by the fact that all the stars are moving, so there isn't any reference point. But that's OK, that is what graduate students were invented for. What is generally given in a star catalog is the Annual Proper Motion, how many seconds of arc a star moves in one year. This is symbolized by the greek letter Mu . The largest known proper motion is Barnard's Star ( often known as Barnard's Runaway Star ) with an mu of 10.2 seconds per year.
The direction a star appears to be moving on the sky is called, surprise, surprise, the Direction of Proper Motion ( sometimes called the Direction Angle of Proper Motion ). It is in degrees. It is measured clockwise, and zero is north.
In the Gliese 3.0 data, Proper Motion is in the field of bytes 31-36,
Radial Velocity is in bytes 44-49, and Direction Angle of Proper Motion is
in bytes 38-42.
pmRA = muRA COS(Dec)where muRA, muDec, pmRA and pmDec are measured in arcsec/yr.
pmDec = muDec
pmRA = pm SIN(pmPA)where pm, pmRA and pmDec are measured in arcsec/yr.
pmDec = pm COS(pmPA)
(1c) Alternatively, you may be given pmRA and pmDec directly. They are provided in the Hipparcos catalogue, so you can skip steps 1a/1b.
(2) Obtain the components of the "space velocity" of the star in the east, north and radially outward directions by dividing the proper motions by the star's parallax (given in arcseconds), this converts the star's velocity from arcsec/year to AU/year. We also multiply by 4.7406 which converts the from AU/year to kilometres/second (1 AU/yr = 4.7406 km/sec).
VE = 4.7406 pmRA / parallaxwhere RV is the radial velocity.
VN = 4.7406 pmDec / parallax
VR = RV
(3) Find the space velocity in rectangular equatorial coordinates.
Vx = VN (-COS RA SIN Dec) + VE (-SIN RA) + VR (COS RA COS Dec)(4) Rotate these velocities into galactic coordinates.
Vy = VN (-SIN RA SIN Dec) + VE (-COS RA) + VR (SIN RA COS Dec)
Vz = VN ( COS Dec) + VR (SIN Dec)
U = -0.0548755 Vx - 0.8734371 Vy - 0.4838350 Vz(5) Convert these velocities from km/s to ly/year or pc/year:
V = 0.4941095 Vx - 0.4448296 Vy + 0.7469822 Vz
W = -0.8676661 Vx - 0.1980764 Vy + 0.4559838 Vz
1 km/s = 3.3355E-6 ly/year
1 km/s = 1.0226E-6 pc/year
Proper motion (RA direction): pmRA = -0.798 arcsec/yrConclusion: Barnard's star is rapidly heading towards us at a velocity of 0.47 light years per millennium.
Proper motion (Dec direction): pmDec= 10.327 arcsec/yr
Radial velocity: RV = -111.0 km/s
Parallax: plx = 0.5490 arcseconds
Right Ascension (2000) RA = 17 57.8 = 269.45 deg
Declination (2000) Dec = +04 41.6 = 4.69 deg
(2) VE = 4.7406 * -0.798 / 0.549
= -6.891 km/s
VN = 4.7406 * 10.327 / 0.549
= +89.171 km/s
VR = -111.0 km/s
(3) Vx = +89.171 (-COS 269.45 SIN 4.69) - 6.891 (-SIN 269.45)
- 111.0 (COS 269.45 COS 4.69)
= -5.76 km/s
Vy = +89.171 (-SIN 269.45 SIN 4.69) - 6.891 (-COS 269.45)
- 111.0 (SIN 269.45 COS 4.69)
= +117.85 km/s
Vz = +89.171 ( COS 4.69) - 111.0 * (SIN 4.69)
= 79.80 km/s
(4) U = -0.0548755 (-5.76) - 0.8734371 (117.85) - 0.4838350 (79.80)
= -141.2 km/s
V = 0.4941095 (-5.76) - 0.4448296 (117.85) + 0.7469822 (79.80)
= +4.3 km/s
W = -0.8676661 (-5.76) - 0.1980764 (117.85) + 0.4559838 (79.80)
= +18.0 km/s
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